Abstract

The determination of the injection composition of cosmic ray nuclei within astrophysical sources requires sufficiently accurate descriptions of the source physics and the propagation – apart from controlling astrophysical uncertainties. We therefore study the implications of nuclear data and models for cosmic ray astrophysics, which involves the photo-disintegration of nuclei up to iron in astrophysical environments. We demonstrate that the impact of nuclear model uncertainties is potentially larger in environments with non-thermal radiation fields than in the cosmic microwave background. We also study the impact of nuclear models on the nuclear cascade in a gamma-ray burst radiation field, simulated at a level of complexity comparable to the most precise cosmic ray propagation code. We conclude with an isotope chart describing which information is in principle necessary to describe nuclear interactions in cosmic ray sources and propagation.

Highlights

  • Particles from space reaching the Earth with energies higher than 109 GeV are detected by ultra-high energy cosmic ray (UHECR) observatories such as the Pierre Auger Observatory[1] and the Telescope Array (TA) experiment[2]

  • UHECRs are expected to be accelerated in astrophysical sources, such as Gamma-Ray Bursts (GRBs; see ref. 26 for a review), Active Galactic Nuclei (AGNs), starburst galaxies, or jets produced in other cataclysmic events – to name a few examples

  • Note that in astrophysical environments, unstable isotopes gain importance, since all kinds of secondary nuclei are created in the disintegration chain and their lifetime is dilated by the relativistic boost

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Summary

Introduction

Particles from space reaching the Earth with energies higher than 109 GeV are detected by ultra-high energy cosmic ray (UHECR) observatories such as the Pierre Auger Observatory[1] and the Telescope Array (TA) experiment[2]. A more sophisticated approach, based on the TALYS nuclear reaction program[22], is implemented in the cosmic ray propagation software CRPropa[2] and 323, 24, which includes 183 isotopes and 2200 channels for the photo-disintegration.

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